SAKMANN AND NEHER INVENT PATCH-CLAMPING Flashcards
A method to measure the behavior of a single ion channel
SAKMANN AND NEHER
PATCH-CLAMPING
Erwin Neher and Bert Sakmann invented a new technique called patch
clamping, which allowed them to study the
behavior of a single ion channel
1991 Nobel Prize in Medicine or Physiology
Neher and
Sakmann
The ion channel is
inserted in the
membrane that is
in the lumen of the electrode,
However, whether
open for a longer or shorter period, the conductance of the Na channel (the amount of current passed
during any instant in time) is always the same. T/F
True
individual channel opens and closes
very rapidly
channels have ___ conductances
unitary
If the same depolarizing pulse was presented a
second time, or a third or fourth time, the same inward current pattern was evoked. This pattern
of current flowing through the entire axon is called the
macroscopic current
patterns of inward current evoked in a single Na channel, called the
microscopic current,
The opening and closing of an individual channel was variable because the behavior of any
channel is
probabilistic.
What the membrane potential does is to change the ___that a
channel will open.
probability
In the case of the Na channel, depolarization increases the probability that the
activation gate will open.
hyperpolarization
increases the probability of
closing the Na activation gate
depolarization increases the probability that the inactivation gate will
close
hyperpolarization
increases the probability that the inactivation gate will
open
How then do we reconcile the stereotyped current response of the squid giant axon to a
depolarization of -10 mV, the shape of the macroscopic current, with the highly variable
response of an individual Na channel, the microscopic current, to exactly the same
depolarization?
squid giant
axon during voltage clamp shows the summated (or averaged) currents through many ion
channels in the entire membrane of the axon rather than the current through a single channel.
was simple to calculate
the probability of a Na channel opening as a function of
membrane potential
function of membrane potential. That function is shown in Fig. 4E, and has a \_\_\_shape
sigmoidal
inward currents are
shown as
downward deflections
Current through a single
channel is called the
microscopic
current
The sum of many such microscopic currents shows that most channels open in the initial\_\_\_after which the probability of channel openings diminishes because of channel inactivation.
1-2 ms,
The macroscopic
current resulting from the current
flowing through all of the Na channels
while
voltage clamping the entire axon
is very similar
to the summed microscopic current in C.
macroscopic current
The probability of Na channel
opening depends on the
membrane
potential,
Notice that the
probability is virtually zero (few or no
channels open) at
-60 to -80 mV
probability of channel opening is about
80% even when the membrane is
depolarized to
+40 mV
Depolarizing steps cause outward currents which are seen as
(upward
deflections
Notice that the K channel opens with different
latencies to the depolarization and that the channels
stay open for the length of the
depolarization,
the probability-membrane
potential function is similar to both the K
conductance-membrane potential function and to the
Na conductance-membrane potential function
T/F
T
Strong hyperpolarization virtually ensures that
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activation gates are closed, since the probability of a Na or K channel being open at ____
is just about zero (
-70-80 mV
the open probability increases
sharply with depolarization at these values
-40 to 0 mV
max probability at
+30 mV.
What is somewhat surprising however is that the maximum open probability is not 100%
but rather only
70-80%
hyperpolarization
guarantees gate closure whereas depolarization only makes gate opening more likely. T/F
T
he probability that the channel can pass Na+ ions decreases after the
depolarization
been present for a period of time due to the closure of the inactivation gate
The delayed closure can be appreciated from the records in Fig. 2 and Fig. 4B, since there were
no channel openings after the first
first 8.0 msec or so of the depolarizing pulse.
It has been known that if a nerve axon is hyperpolarized for a period of time, an
action potential is often set off when the hyperpolarization is released and the cell quickly
brought back to rest; this is called
anode break excitation or rebound excitation.
explanation for rebound excitation is that
hyperpolarization of the membrane increases
the number of Na channels available for opening in response to depolarization
why the states of the activation and
inactivation gates are “probabilistic”.
This “flickering” between states
even when the membrane potential is not changing,